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From Discovery to the First Month of the Type II Supernova 2023ixf: High and Variable Mass Loss in the Final Year Before Explosion

Authors :
Hiramatsu, Daichi
Tsuna, Daichi
Berger, Edo
Itagaki, Koichi
Goldberg, Jared A.
Gomez, Sebastian
De, Kishalay
Hosseinzadeh, Griffin
Bostroem, K. Azalee
Brown, Peter J.
Arcavi, Iair
Bieryla, Allyson
Blanchard, Peter K.
Esquerdo, Gilbert A.
Farah, Joseph
Howell, D. Andrew
Matsumoto, Tatsuya
McCully, Curtis
Newsome, Megan
Gonzalez, Estefania Padilla
Pellegrino, Craig
Rhee, Jaehyon
Terreran, Giacomo
Vinkó, József
Wheeler, J. Craig
Publication Year :
2023

Abstract

We present the discovery of Type II supernova (SN) 2023ixf in M101, among the closest core-collapse SNe in the last several decades, and follow-up photometric and spectroscopic observations in the first month of its evolution. The light curve is characterized by a rapid rise ($\approx5$ days) to a luminous peak ($M_V\approx-18$ mag) and plateau ($M_V\approx-17.6$ mag) extending to $30$ days with a smooth decline rate of $\approx0.03$ mag day$^{-1}$. During the rising phase, $U-V$ color shows blueward evolution, followed by redward evolution in the plateau phase. Prominent flash features of hydrogen, helium, carbon, and nitrogen dominate the spectra up to $\approx5$ days after first light, with a transition to a higher ionization state in the first $\approx2$ days. Both the $U-V$ color and flash ionization states suggest a rise in the temperature, indicative of a delayed shock-breakout inside dense circumstellar material (CSM). From the timescales of CSM interaction, we estimate its compact radial extent of $\sim(3-7)\times10^{14}$ cm. We then construct numerical light-curve models based on both continuous and eruptive mass-loss scenarios shortly before explosion. For the continuous mass-loss scenario, we infer a range of mass-loss history with $0.1-1.0$ $M_\odot {\rm yr}^{-1}$ in the final $2-1$ years before explosion, with a potentially decreasing mass loss of $0.01-0.1$ $M_\odot {\rm yr}^{-1}$ in $\sim0.7-0.4$ years towards the explosion. For the eruptive mass-loss scenario, we favor eruptions releasing $0.3-1$ $M_\odot$ of the envelope at about a year before explosion, which result in CSM with mass and extent similar to the continuous scenario. We discuss the implications of the available multi-wavelength constraints obtained thus far on the progenitor candidate and SN 2023ixf to our variable CSM models.<br />15 pages, 5 figures, submitted to ApJL

Details

Language :
English
Database :
OpenAIRE
Accession number :
edsair.doi.dedup.....e93ae2f6d620b1b14646abefff7ba01f